Field data on the rates of solifluction and associated parameters are compi
led from the literature, in an attempt to evaluate factors controlling the
spatial variability in solifluction processes and landforms, with special a
ttention on the climate-solifluction. relationship. The analyzed data origi
nate from 46 sites over a wide range of periglacial environments, from Anta
rctic nunataks to tropical high mountains. Solifluction, broadly defined as
slow mass wasting resulting from freeze-thaw action in fine-textured soils
, involves several components: needle ice creep and diurnal frost creep ori
ginating from diurnal freeze-thaw action; annual frost creep, gelifluction
and plug-like flow originating from annual freeze-thaw action; and retrogra
de movement caused by soil cohesion. The depth and thickness of ice lenses
and freeze-thaw frequency are the major controls on the spatial variation i
n solifluction processes. Near the warm margin of the solifluction-affected
environment, diurnal freeze-thaw action induces shallow but relatively rap
id movement of a superficial layer 5 - 10 cm thick on average, often creati
ng the thin stone-banked lobes typically seen on tropical high mountains. I
n addition to diurnal movement, annual frost creep and gelifluction may occ
ur on slopes with soil climates of seasonal frost to warm permafrost, dislo
cating a soil layer shallower than 60 cm at a rate of centimeters per year
and eventually producing medium-size solifluction lobes. In High-Arctic col
d permafrost regions, two-sided freezing can induce plug-like flow of a soi
l mass 60 cm or thicker. The correlation between process and landform. sugg
ests that the riser height of lobes is indicative of the maximum depth of m
ovement and prevailing freeze-thaw type. Climate change may result in new d
ifferent ground freezing conditions, thereby influencing the surface veloci
ty and maximum depth of soil movement. Soil moisture and topography also co
ntrol solifluction. High moisture availability in the seasonal freezing per
iod enhances diurnal freeze-thaw action and subsequent seasonal frost heavi
ng. The latter contributes to raising the moisture content of the thawed la
yer and promotes gelifluction during the thawing period. The slope angle de
fines the upper limit of the surface velocity of solifluction. A diagram co
rrelating the potential frost creep with the actual surface velocity permit
s an inter-site comparison of the relative magnitude of solifluction compon
ents. Physically based modelling of periglacial slope evolution requires sy
nthetic and more detailed field monitoring and laboratory simulations of so
lifluction processes. (C) 2001 Elsevier Science B.V. All rights reserved.